Bi2Er: enthalpy of formation
23 accepted literature formation-enthalpy value(s) (model 21, DFT 2); OQMD -46.37 kJ/mol-atom (oqmd-1800946).
Systems: Bi–Er
Literature values
| Value | Phase as printed | T (K) | Class | Method | System | Source | Location | Quote |
|---|---|---|---|---|---|---|---|---|
| -59 kJ/mol-atom | ErBi2 | model | Miedema model | Bi–Er | [1] Bennoui 2022 cites Colinet 1984 doi | Table 2, p. 5, row 3 report | ||
| -53.528 kJ/mol-atom | ErBi2 | model | CALPHAD | Bi–Er | [1] Bennoui 2022 | Table 2, p. 5, row 2 report | ||
| -48.2365 kJ/mol-atom | ErBi2 (NdAs2-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 19 report | ||
| -47.7533 kJ/mol-atom | ErBi2 (SmSb2-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 18 report | ||
| -45.9664 kJ/mol-atom | ErBi2 (CaSb2-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 17 report | ||
| -45.2102 kJ/mol-atom | ErBi2 | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 16 report | ||
| -45.1803 kJ/mol-atom | ErBi2 (Co2Si-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 15 report | ||
| -43.6048 kJ/mol-atom | ErBi2 (LaAs2-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 14 report | ||
| -43.2532 kJ/mol-atom | ErBi2 (ErTe2-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 13 report | ||
| -38.4406 kJ/mol-atom | ErBi2 (Al2Cu-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 12 report | ||
| -35.9422 kJ/mol-atom | ErBi2 (AuTe2-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 11 report | ||
| -33.6478 kJ/mol-atom | ErBi2 (MoSi2-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 10 report | ||
| -25.414 kJ/mol-atom | ErBi2 (FeS2-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 9 report | ||
| -25.1344 kJ/mol-atom | ErBi2 (Fe2P-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 8 report | ||
| -23.4701 kJ/mol-atom | ErBi2 (MoS2-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 7 report | ||
| -23.1992 kJ/mol-atom | ErBi2 (CoSi2-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 6 report | ||
| -21.1173 kJ/mol-atom | ErBi2 (Ag2Se-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 5 report | ||
| -16.5698 kJ/mol-atom | ErBi2 (ErSb2-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 4 report | ||
| -15.4151 kJ/mol-atom | ErBi2 (FeS2-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 3 report | ||
| 15.2241 kJ/mol-atom | ErBi2 (MoS2-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 2 report | ||
| 39.6679 kJ/mol-atom | ErBi2 (CdI2-type) | 0 | model | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 1 report | ||
| -45.237 kJ/mol-atom | ErBi2 | 0 | DFT | DFT | Bi–Er | [1] Bennoui 2022 | Table 2, p. 5, row 1 report | |
| -45.2102 kJ/mol-atom | ErBi2 (ErSn2-type) | 0 | DFT | Bi–Er | [1] Bennoui 2022 | Table 3, p. 6, row 16 report |
Uncertainty budget
Components kept separate, in the value's unit (literature SCHEMA.md, UNCERTAINTY_CALIBRATION.md): effective = max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter). The method floor is the robust between-study scatter of the method class in ORCHID (calibrated) or a documented prior; printed values and printed uncertainties are unchanged.
| Value | Unit | Printed | Reading | Method (class, basis) | Composition | Scatter | Conversion | Effective |
|---|---|---|---|---|---|---|---|---|
| -59 | kJ/mol-atom | 0.05 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -53.528 | kJ/mol-atom | 5.000e-4 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -48.2365 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -47.7533 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -45.9664 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -45.2102 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -45.1803 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -43.6048 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -43.2532 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -38.4406 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -35.9422 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -33.6478 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -25.414 | kJ/mol-atom | 5.000e-4 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -25.1344 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -23.4701 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -23.1992 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -21.1173 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -16.5698 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -15.4151 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| 15.2241 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| 39.6679 | kJ/mol-atom | 5.000e-5 | 3.9 (model_calculated, calibrated) | 3.9 | ||||
| -45.237 | kJ/mol-atom | 5.000e-4 | 8.395 (dft, calibrated) | 8.395 | ||||
| -45.2102 | kJ/mol-atom | 5.000e-5 | 8.395 (dft, calibrated) | 8.395 |
DFT formation energies
Lowest-energy entries at this composition. Materials Project and OQMD use different energy references and are never averaged. 1 eV/atom = 96.485 kJ/mol-atom.
| Source | Entry | kJ/mol-atom | eV/atom | Space group | E above hull (kJ/mol-atom) | E above hull (eV/atom) | Theoretical |
|---|---|---|---|---|---|---|---|
| OQMD | oqmd-1039322 | -38.396 | -0.397943 | I4/mcm | 15.2524 | 0.1581 | yes |
| OQMD | oqmd-1040064 | -33.717 | -0.349458 | I4/mmm | 19.9305 | 0.2066 | yes |
| OQMD | oqmd-1800946 | -46.37 | -0.48059 | P21/m | 7.2781 | 0.0754 | yes |
DFT sources: A. Jain et al., Commentary: The Materials Project: A materials genome approach to accelerating materials innovation, APL Materials 1 (2013) 011002. doi:10.1063/1.4812323 (CC BY 4.0); J. E. Saal et al., JOM 65 (2013) 1501-1509; S. Kirklin et al., npj Comput. Mater. 1 (2015) 15010. doi:10.1007/s11837-013-0755-4 (CC BY 4.0);
Sources
- S. Bennoui, Y. Djaballah, V. Vassiliev, A. Belgacem-Bouzida, Thermodynamic Study of Er-Bi and Er-Te Systems by Combination of First-Principles Calculations and the CALPHAD Method, J. Phase Equilib. Diffus. 43, 126-138 (2022). doi:10.1007/s11669-022-00947-8